NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = R.Brissot Found 38 matches. 1991BE33 Phys.Rev.Lett. 67, 3661 (1991) M.Bernas, P.Armbruster, S.Czajkowski, H.Faust, J.P.Bocquet, R.Brissot Discovery of Neutron-Rich Co and Fe Isotopes in 239Pu(n(th), f): Yields and half-lives NUCLEAR REACTIONS 239Pu(n, F), E=thermal; measured fission fragment mass, isotopic yields, (fragment)β(t). 69,68Co, 68Fe deduced T1/2.
doi: 10.1103/PhysRevLett.67.3661
1990BE13 Z.Phys. A336, 41 (1990) M.Bernas, P.Armbruster, J.P.Bocquet, R.Brissot, H.Faust, Ch.Kozhuharov, J.L.Sida Beta-Decay Half-Lives of Neutron Rich Cu and Ni Isotopes Produced by Thermal Fission of 235U and 239Pu NUCLEAR REACTIONS 235U, 239Pu(n, F), E=thermal; measured fission fragment elemental distributions; deduced evidence for 74,75Cu, 71,72,73Ni. Magnetic, electrostatic analysis. RADIOACTIVITY 74,75Cu, 71,72,73Ni [from 235U, 239Pu(n, F), E=thermal]; measured β-decay T1/2. Model comparison. Planar Si detectors.
1990BO05 Z.Phys. A335, 41 (1990) J.P.Bocquet, R.Brissot, H.R.Faust, M.Fowler, J.Wilhelmy, M.Asghar, M.Djebara Characteristics of Mass and Nuclear Charge Distributions of 229Th(n(th), F). Implications for Fission Dynamics NUCLEAR REACTIONS 229Th(n, F), E=thermal; measured fission fragment yield vs mass, charge; deduced proton odd-even effect role in fission. Other data analyzed. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22143. 1990MA49 Nucl.Phys. A515, 433 (1990) G.Martinez, G.Barreau, A.Sicre, T.P.Doan, P.Audouard, B.Leroux, W.Arafa, R.Brissot, J.P.Bocquet, H.Faust, P.Koczon, M.Mutterer, F.Gonnenwein, M.Asghar, U.Quade, K.Rudolph, D.Engelhardt, E.Piasecki Mass and Nuclear Charge Yields for 237Np(2n(th), f) at Different Fission Fragment Kinetic Energies NUCLEAR REACTIONS 239Np(n, F), E=thermal; measured light fission product mass versus kinetic energies; deduced fractional independent fission yields, odd-even effects of elements, isotones. Double neutron capture on 237Np target.
doi: 10.1016/0375-9474(90)90593-B
1989BO36 Nucl.Phys. A502, 213c (1989) Mass, Energy and Nuclear Charge Distribution of Fission Fragments NUCLEAR STRUCTURE A=229-249; compiled thermal neutron induced fission data analyses; deduced fragment yield fine structure, charge distribution features.
doi: 10.1016/0375-9474(89)90663-5
1989DJ01 Nucl.Phys. A496, 346 (1989) M.Djebara, M.Asghar, J.P.Bocquet, R.Brissot, J.Crancon, Ch.Ristori, E.Aker, D.Engelhardt, J.Gindler, B.D.Wilkins, U.Quade, K.Rudolph Mass and Nuclear-Charge Yields for 249Cf(n(th), F) at Different Fission-Product Kinetic Energies NUCLEAR REACTIONS 249Cf(n, F), E=thermal; measured light fission product mass, nuclear-charge distributions vs kinetic energies; deduced fractional independent yields, odd-even effects, mean kinetic energies of masses, elements and isotones.
doi: 10.1016/0375-9474(89)90179-6
1989SI22 Nucl.Phys. A502, 233c (1989) J.L.Sida, P.Armbruster, M.Bernas, J.P.Bocquet, R.Brissot, H.R.Faust Mass, Charge, and Energy Distributions in Very Asymmetric Thermal Fission of 235U NUCLEAR REACTIONS 235U(n, F), E=thermal; measured fission fragment mass, charge, energy distributions; deduced fission features.
doi: 10.1016/0375-9474(89)90664-7
1987AR21 Europhys.Lett. 4, 793 (1987) P.Armbruster, M.Bernas, J.P.Bocquet, R.Brissot, H.R.Faust, P.Roussel Identification of the New Neutron-Rich Isotopes 70-74Ni and 74-77Cu in Thermal Neutron Fission of 235U NUCLEAR REACTIONS 235U(n, F)70Ni/71Ni/72Ni/73Ni/74Ni/74Cu/75Cu/76Cu/77Cu, E=thermal; measured fission fragment yields. Recoil separator, ΔE-E detection.
doi: 10.1209/0295-5075/4/7/006
1987BO24 Nucl.Phys. A470, 13 (1987) M.Bogdanovic, R.Brissot, G.Barreau, K.Schreckenbach, S.Kerr, H.G.Borner, I.A.Kondurov, Yu.E.Loginov, V.V.Martynov, P.A.Sushkov, H.Seyfarth, T.von Egidy, P.Hungerford, H.H.Schmidt, H.J.Scheerer, A.Chalupka, W.Kane, G.Alaga The Level Scheme of 134Cs NUCLEAR REACTIONS 133Cs(n, γ), E=thermal, 5.9 eV, 22.6 eV; measured Eγ, Iγ, I(ce), γγ-coin. 133Cs(d, p), E=12 MeV; analyzed data. 134Cs deduced levels, J, π, ICC, γ-multipolarity, configurations. Curved-crystal spectrometers, magnetic spectrometer, pair spectrometer, neutron monochromator, enriched targets.
doi: 10.1016/0375-9474(87)90119-9
1986AK04 Radiat.Eff. 93, 1 (1986) E.Aker, D.Engelhardt, R.Brissot, P.Brissot, P.Geltenbort, F.Gonnenwein, A.Oed, J.Gindler, B.Wilkins Mass and Energy Distribution of Fission Fragments in 249Cf(n(th), f) NUCLEAR REACTIONS 249Cf(n, F), E=thermal; measured fission fragment mass, energy distribution; deduced relative mass yields.
doi: 10.1080/00337578608207415
1986AS01 Radiat.Eff. 93, 69 (1986) M.Asghar, J.P.Bocquet, R.Brissot, M.Djebara, M.Maurel, H.Nifenecker, Ch.Ristori Quasi-Particle Excitations in Low Energy Fission NUCLEAR REACTIONS 229Th, 232U(n, F), E=thermal; measured fission fragment yield vs mass; deduced proton odd-even effect. 230Th, 233U deduced quasiparticle excitations.
doi: 10.1080/00337578608207432
1986WA05 Phys.Rev. C33, 943 (1986) C.Wagemans, P.D'hondt, P.Schillebeeckx, R.Brissot Triton and Alpha Emission in the Thermal-Neutron-Induced Ternary Fission of 233U, 235U, 239Pu, and 241Pu NUCLEAR REACTIONS 233,235U, 239,241Pu(n, αF), (n, tF), (n, α), E=thermal; measured ternary fission α-, triton yield, energy distributions; deduced σ(n, α0) upper-limit.
doi: 10.1103/PhysRevC.33.943
1984DH05 Ann.Nucl.Energy 11, 485 (1984) P.D'Hondt, C.Wagemans, A.Emsallem, R.Brissot Measurement of the Thermal-Neutron-Induced Fission Cross-Section of 238U NUCLEAR REACTIONS 238U(n, F), E=thermal; measured fission fragment spectra, fission σ relative to 235U. 239U deduced negative energy resonances.
doi: 10.1016/0306-4549(84)90073-2
1984DJ02 Nucl.Phys. A425, 120 (1984) M.Djebara, M.Asghar, J.P.Bocquet, R.Brissot, M.Maurel, H.Nifenecker, Ch.Ristori Measurement of Charge Distributions for 229Th(n(th), f) and 232U(n(th), f) NUCLEAR REACTIONS 229Th, 232U(n, F), E=thermal; measured fission fragment charge yields, correlations with kinetic energy; deduced yields, most probable kinetic energies odd-even effect.
doi: 10.1016/0375-9474(84)90219-7
1984MH01 Nucl.Phys. A412, 113 (1984) A.Mheemeed, K.Schreckenbach, G.Barreau, H.R.Faust, H.G.Borner, R.Brissot, P.Hungerford, H.H.Schmidt, H.J.Scheerer, T.Von Egidy, K.Heyde, J.L.Wood, P.Van Isacker, M.Waroquier, G.Wenes, M.L.Stelts The Level Structure of 114Cd from (n, γ) and (d, p) Studies NUCLEAR REACTIONS 113Cd(n, γ), E=thermal, 2 keV, 24 keV; 113Cd(n, e-), E=thermal; 113Cd(d, p), E=10 MeV; measured Eγ, Iγ, I(ce), E(p), σ(E(p)). 114Cd deduced levels, J, π, ICC, γ-branching, E0 branches. Curved crystal spectrometers, Ge(Li) pair spectrometers, magnetic conversion electron spectrometer, magnetic spectrograph, enriched targets. Comparison with proton 2p-2h coupling, interacting boson model configuration mixing calculations.
doi: 10.1016/0375-9474(84)90388-9
1984OE01 Nucl.Instrum.Methods 219, 569 (1984) A.Oed, P.Geltenbort, R.Brissot, F.Gonnenwein, P.Perrin, E.Aker, D.Engelhardt A Mass Spectrometer for Fission Fragments Based on Time-of-Flight and Energy Measurements NUCLEAR REACTIONS 235U(n, F), E=thermal; measured fission fragment energy spectra; deduced fission fragment mass resolving power. Tof detectors, ionization chambers.
doi: 10.1016/0167-5087(84)90232-1
1984SC38 Nucl.Phys. A430, 21 (1984) C.Schmitt, A.Guessous, J.P.Bocquet, H.-G.Clerc, R.Brissot, D.Engelhardt, H.R.Faust, F.Gonnenwein, M.Mutterer, H.Nifenecker, J.Pannicke, Ch.Ristori, J.P.Theobald Fission Yields at Different Fission-Product Kinetic Energies for Thermal-Neutron-Induced Fission of 239Pu NUCLEAR REACTIONS 239Pu(n, F), E=thermal; measured fission fragment mass, charge distribution; deduced fragment fractional yields, odd-even effects, isobar average kinetic energies.
doi: 10.1016/0375-9474(84)90191-X
1984VO01 J.Phys.(London) G10, 221 (1984) T.von Egidy, H.Daniel, P.Hungerford, H.H.Schmidt, K.P.Lieb, B.Krusche, S.A.Kerr, G.Barreau, H.G.Borner, R.Brissot, C.Hofmeyr, R.Rascher Levels and Gamma Transitions of 40K Studied by Neutron Capture NUCLEAR REACTIONS 39K(n, γ), E=thermal; measured Eγ, Iγ. 40K deduced neutron binding energy, levels, J, π, γ-branching. Shell, statistical models.
doi: 10.1088/0305-4616/10/2/013
1983BE05 Z.Phys. A309, 253 (1983) D.Belhafaf, J.P.Bocquet, R.Brissot, Ch.Ristori, J.Crancon, H.Nifenecker, J.Mougey, V.S.Ramamurthy Kinetic Energy Distributions around Symmetric Thermal Fission of U234 and U236 NUCLEAR REACTIONS 233,235U(n, F), E=thermal; measured fission fragment kinetic energy vs mass. 234,236U deduced symmetric fission characteristics.
doi: 10.1007/BF01413757
1983TO20 Nucl.Phys. A411, 209 (1983) Y.Tokunaga, H.Seyfarth, O.W.B.Schult, H.G.Borner, Ch.Hofmeyr, G.Barreau, R.Brissot, U.Kaup, Ch.Monkemeyer The 75Se(n, γ)76Se Reaction and the Low-Lying Level Structure of 76Se NUCLEAR REACTIONS 75Se(n, γ), E=thermal; measured σ, Iγ, Eγ. 76Se deduced levels J, π, neutron binding energy. Enriched target. Interacting boson models.
doi: 10.1016/0375-9474(83)90389-5
1982KR12 Nucl.Phys. A386, 245 (1982) B.Krusche, K.P.Lieb, H.Daniel, T.von Egidy, G.Bareau, H.G.Borner, R.Brissot, C.Hofmeyr, R.Rascher Gamma Ray Energies and 36Cl Level Scheme from the Reaction 35Cl(n, γ) NUCLEAR REACTIONS 35Cl(n, γ), E=thermal; measured Eγ, Iγ. 36Cl deduced levels, neutron binding energy. Crystal, pair spectrometers.
doi: 10.1016/0375-9474(82)90112-9
1982SC09 Phys.Lett. 110B, 364 (1982) K.Schreckenbach, A.Mheemeed, G.Barreau, T.von Egidy, H.R.Faust, H.G.Borner, R.Brissot, M.L.Stelts, K.Heyde, P.van Isacker, M.Waroquier, G.Wenes The Importance of Intruder States in 114Cd NUCLEAR REACTIONS 113Cd(n, γ), (n, e-), E=thermal; 113Cd(n, γ), E=2, 24 keV; measured Eγ, Iγ, I(ce). 114Cd deduced levels, γ-branching ratio, J, π, T1/2, B(E0), B(E2). Two-particle, two-hole core coupling calculations.
doi: 10.1016/0370-2693(82)91273-4
1982SC14 Phys.Rev. C25, 2888 (1982) H.H.Schmidt, P.Hungerford, H.Daniel, T.von Egidy, S.A.Kerr, R.Brissot, G.Barreau, H.G.Borner, C.Hofmeyr, K.P.Lieb Levels and Gamma Energies of 28Al Studied by Thermal Neutron Capture NUCLEAR REACTIONS 27Al(n, γ), E=thermal; measured Eγ, Iγ. 28Al deduced levels, J, π, neutron binding energy. Cyrstal spectrometer, Ge(Li) detector. RADIOACTIVITY 28Al [from 27Al(n, γ), E=thermal]; measured Eγ, Iγ following β-decay. 28Si deduced transition energy. Crystal spectrometer, Ge(Li) detector.
doi: 10.1103/PhysRevC.25.2888
1981BO42 Fizika(Zagreb) 13, Suppl.No.2, 40 (1981) M.Bogdanovic, R.Brissot, G.Barreau, K.Schreckenbach, S.Kerr, I.A.Kondurov, Yu.E.Loginov, V.V.Martynov, P.A.Sushkov The Level Structure of 134Cs NUCLEAR REACTIONS 133Cs(n, γ), E=thermal; measured Eγ, Iγ, I(ce), γγ-coin. 134Cs deduced levels, J, π, configuration, γ-transition multipolarity.
1981MA03 Nucl.Instrum.Methods 180, 141 (1981) G.Mariolopoulos, J.P.Bocquet, R.Brissot, H.Nifenecker, Ch.Ristori, A.Pequet, J.Girard A New Experimental Method to Measure the Charge Distributions of Fission Products RADIOACTIVITY, Fission 252Cf(SF); measured (fragment)(X-ray)-coin, fragment charge distribution; deduced yields for Rb, Sr, Y, Zr, Nb, Mo, Tc, Ru, Rh, Pd, Ag. ΔE-E telescope, X-ray detector.
doi: 10.1016/0029-554X(81)90021-5
1981MA07 Nucl.Phys. A361, 213 (1981) G.Mariolopoulos, Ch.Hamelin, J.Blachot, J.P.Bocquet, R.Brissot, J.Crancon, H.Nifenecker, Ch.Ristori Charge Distributions in Low-Energy Nuclear Fission and Their Relevance to Fission Dynamics NUCLEAR REACTIONS, Fission 229Th(n, F), E=thermal; 235U(n, F), E=3 MeV; measured fragment charge distribution; deduced strong even-odd effects, pair breaking probability variation from saddle point to scission. RADIOACTIVITY, Fission 252Cf(SF); measured fragment charge distribution.
doi: 10.1016/0375-9474(81)90477-2
1981SU12 Fizika(Zagreb) 13, Suppl.No.2, 39 (1981) P.A.Sushkov, I.A.Kondurov, M.Bogdanovic, T.Mitsunari, T.D.Mac Mahon, H.A.Baader, D.Breitig, R.Koch, H.Seyfarth, O.W.B.Schult, H.Borner, R.Brissot, G.Barreau, H.Faust, K.Schreckenbach The Level Scheme of 110Ag from the (n, γ) Reaction NUCLEAR REACTIONS 109Ag(n, γ), E not given; measured Eγ, Iγ, I(ce), γγ-coin. 110Ag deduced levels, configuration.
1977BR11 Nucl.Phys. A282, 109 (1977) R.Brissot, J.Crancon, C.Ristori, J.P.Bocquet, A.Moussa Distributions Isotopiques des Gaz Rares et de Leurs Precurseurs dans la Fission Thermique de 239,241Pu: Etude de l'Effet 'Pair-Impair' NUCLEAR REACTIONS 239,241Pu(n, F), E=th; measured rare gas fission yields, mass, charge distributions, deduced odd-even effect. On-line isotopic separation of products.
doi: 10.1016/0375-9474(77)90174-9
1977FE03 J.Phys.(Paris) 38, 273 (1977) C.A.Feu Alvim, J.P.Bocquet, R.Brissot, J.Crancon, A.Moussa Mesure, par Une Method d'Emanation, des Rendements des Gaz Rares dans la Fission de 238U et 232Th par Neutrons de 14 MeV NUCLEAR REACTIONS 238U, 232Th(n, F), E=14 MeV; measured Kr, Xe yields, σ(A, Z). Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21567. 1976BR25 J.Phys.(Paris), Lett. 37, L-241 (1976) R.Brissot, J.Crancon, C.Ristori, A.Moussa Distributions Isotopiques des Gaz Rares dans la Fission par Neutrons Thermiques de 239Pu et 241Pu. Evaluation de l'Effet de Parite en Protons NUCLEAR REACTIONS 239,241Pu(n, F), E=th; measured Kr, Xe yields.
doi: 10.1051/jphyslet:019760037010024100
1975BR03 Nucl.Phys. A238, 149 (1975) R.Brissot, F.Schussler, E.Monnand, A.Moussa Niveaux de 93Rb et 93Sr Alimentes dans les Desintegrations β de 93Kr et 93Rb RADIOACTIVITY 93Kr, 93Rb; measured Eβ, Iβ, Eγ, Iγ, βγ-, γγ-coin; deduced log ft. 93Rb, 93Sr deduced levels, J, π.
doi: 10.1016/0375-9474(75)90345-0
1975BR27 Nucl.Phys. A255, 461 (1975) R.Brissot, J.Crancon, C.Ristori, J.P.Bocquet, A.Moussa Distributions Isotopiques des Gaz Rares dans la Fission par Neutrons Thermiques de 235U et 233U NUCLEAR REACTIONS 233U, 235U(n, F), E=thermal; measured independent, cumulative yields of rare gas isotopes; deduced deviations from ucd, widths of gaussian distributions, elemental yields of Br, Kr, Xe. On-line isotopic separation of the products.
doi: 10.1016/0375-9474(75)90693-4
1975MO06 J.Phys.(Paris) 36, 1 (1975) E.Monnand, R.Brissot, J.Crancon, C.Ristori, F.Schussler, A.Moussa Niveaux de 137Cs Alimentes dans la Desintegration de 137Xe RADIOACTIVITY 137Xe; measured Eγ, Iγ, γγ-coin, Iβ; deduced β-branching, log ft. 137Cs deduced levels, γ-branching, T1/2 limit. 138Cs deduced transitions.
doi: 10.1051/jphys:019750036010100
1974SC39 Radiochim.Acta 21, 8 (1974) F.Schussler, P.Cavallini, L.C.Carraz, R.Brissot, J.Crancon, E.Monnand, C.Ristori, A.Moussa Desintegration de 93Sr (T1/2 = 7.3 min). Niveau Isomerique de 93Y (T1/2 = 1.7 sec) RADIOACTIVITY 93Sr; measured Eβ, Eγ, Iγ, γ(t), γγ-coin, βγ-coin; deduced Q, ICC, log ft. 93Y deduced levels, J, π, T1/2.
1973SC18 Nucl.Phys. A209, 589 (1973) F.Schussler, R.Brissot, J.Crancon, E.Monnand, C.Ristori, A.Moussa Desintegration de 140Cs (T1/2 = 64 sec) RADIOACTIVITY 140Cs [from 235U(nth, F)]; measured Eβ, Iβ, Eγ, Iγ, βγ-, γγ-coin, γγ- angular correlations, Q; deduced log ft; 140Ba deduced levels, J, π.
doi: 10.1016/0375-9474(73)90848-8
1972BO25 Nucl.Phys. A189, 556 (1972) J.P.Bocquet, R.Brissot, J.Crancon, A.Moussa On-Line Measurements of Rare-Gas Fission Yields in 14 MeV Neutron Fission NUCLEAR REACTIONS, Fission 233U, 235U, 238U, 232Th(n, F), En=14 MeV; measured independent, cumulative yields of rare-gas isotopes; deduced deviations from UCD, widths of Gaussian distributions. On-line isotopic separation of the products.
doi: 10.1016/0375-9474(72)90314-4
1972MO33 Nucl.Phys. A195, 192 (1972) E.Monnand, R.Brissot, L.C.Carraz, J.Crancon, C.Ristori, F.Schussler, A.Moussa Desintegration de 138Xe RADIOACTIVITY 138Xe[from 235U(n, F)]; measured Eβ, Iβ, I(ce), Eγ, Iγ, βγ-, γγ-coin, T1/2; deduced ICC, log ft, Qβ. 138Cs deduced levels, J, π.
doi: 10.1016/0375-9474(72)90730-0
1969BO02 Nucl.Phys. A125, 613 (1969) J.P.Bocquet, R.Brissot, J.Crancon, J.A.Pinston, F.Schussler, A.Moussa Desintegration du 87Kr RADIOACTIVITY 87Kr [from 235U(n, F)]; measured Eβ, Iβ, Eγ, Iγ, βγ-, γγ-coin. 87Rb deduced levels. Mass separated sources.
doi: 10.1016/0375-9474(69)90751-9
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